Superbubble Feedback in Galaxy Formation Ben Keller (McMaster - - PowerPoint PPT Presentation

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Superbubble Feedback in Galaxy Formation Ben Keller (McMaster - - PowerPoint PPT Presentation

Superbubble Feedback in Galaxy Formation Ben Keller (McMaster University) James Wadsley, Samantha Benincasa, Hugh Couchman Paper: astro-ph/1405.2625 (Accepted MNRAS) Keller, Wadsley, Benincasa & Couchman 2014 Background Image:


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SLIDE 1

Superbubble Feedback in Galaxy Formation

Ben Keller (McMaster University) James Wadsley, Samantha Benincasa, Hugh Couchman Paper: astro-ph/1405.2625 (Accepted MNRAS) Keller, Wadsley, Benincasa & Couchman 2014

Background Image: High-resolution simulation of Milky Way like galaxy using superbubble feedback. Outflows with entrained cold clouds can be observed.

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SLIDE 2

Stellar Feedback: Motivation

M82 Image: HST, NASA/ESA

  • Feedback from Massive

stars: metals, energy, momentum through Winds, UV, SNII

  • FB regulates star

formation, ISM structure FB-driven Galactic winds:

  • Remove gas from disk,

enrich IGM with metals

  • Set final stellar mass
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SLIDE 3

Superbubble Feedback: Motivation

N70 Superbubble LMC Image: ESO D 100 pc Age: 5 Myr v ~ 70 km/s Driver: OB assoc. 1000+ stars

  • Massive star formation

highly correlated in time and space

  • Typical star cluster

~ 10,000 Mʘ forms in ~10 pc over < 1 Myr Stellar Feedback highly correlated Natural unit of feedback is a superbubble combining feedback of 100+ massive stars

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SLIDE 4

Super bubble features

MacLow & McCray 1988, Weaver+ 1977, Silich+ 1996

Classic model:

  • Stellar winds + supernovae

shock and thermalize in bubble

  • Negligible Sedov-phase
  • Mechanical Luminosity

L=1034 erg/s/Mʘ

  • Much more efficient than

individual SN (e.g. Stinson 2006 Blastwave feedback model )

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SLIDE 5

Super bubble features

Limiting factor: Radiative Cooling of bubble determined by bubble temperature ~ Eth/Mb and density Mb/R3 Hot bubble mass (Mb) set by thermal conduction rate into bubble

MacLow & McCray 1988, Weaver+ 1977, Silich+ 1996

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SLIDE 6

Modeling Superbubbles

  • 1. Key physics: Thermal Conduction

Without conduction bubble mass = ejecta mass

  • 2. Evaporation resulting from conduction – hard to

resolve directly

  • 3. Low resolution, early bubble stages:

Mb < Mparticle – need to avoid overcooling

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SLIDE 7
  • 1. Thermal Conductivity
  • Self regulating Energy flux ~ T7/2/R (T > 105 K)
  • Flux limited by electron speeds (Cowie & McKee

1977)

  • Note: κ reduced by 3-5 by Magnetic Fields
  • For sharp temperature contrast, drives evaporative

mass flux from cold into hot gas

(cgs) 10 6 ) (

2 / 5 7 T

T t E

Cond Cond 

        

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SLIDE 8
  • 2. Evaporation
  • Evaporation front width < 0.1

pc ! Subgrid model:

  • Based on MacLow & McCray

1988 rate estimate

  • SPH implemention:

Stochastically evaporate particles into hot bubble from cold shell

  • Applied for T > 105 K particles
  • Regulates bubble temperature

2 / 5

25 16 T k t M

b b

    

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SLIDE 9
  • 3. Low Resolution : Subgrid Hot Phase
  • For a poorly resolved bubble, Mb < Mparticle for

the early stages

  • Temporary 2-phase particle while

injection/conduction grows mass of bubble phase

  • No numerical/resolution related overcooling
  • Feedback-heated particles briefly contain 2

phases in pressure equilibrium, with separate densities and temperatures

– Each cools independently.

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SLIDE 10
  • N-body Solver (Tree Method) and

Smoothed Particle Hydrodynamics

  • Physics: Gravity, Hydrodynamics, Atomic

Chemistry (Radiative Heating, Cooling), Radiative Transfer (Woods et al, in prep)

  • Subgrid Physics: Star Formation,

Turbulent Diffusion

Gasoline

Implementation:

Wadsley+ 2004

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SLIDE 11

High Resolution Superbubble Simulation

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SLIDE 12

Mass loading

  • Bubble mass, temperature regulated:

Match Silich+ 1996 Mass loading For 3x1038 erg/s Feedback

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SLIDE 13

Test 30,000 Mʘ cluster: 3 cases

Direct Injection: Resolved stellar ejecta mass, no subgrid required (Mparticle=760 Mʘ at 1283), conduction + evaporation Superbubble: conduction, evaporation + subgrid Simple Feedback: A non-cooling phase with conversion time 5 Myr to cooling form (cf. Agertz+ 2013)

Keller+ 2014

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SLIDE 14

Bubble Momentum + Hot Mass

  • Simple Model resolution sensitive
  • Superbubble Model still works with a 1 particle bubble

(323 case)

Keller+ 2014

Time (Myr) Hot Bubble Mass Bubble Momentum

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SLIDE 15

Galaxy Tests

Similar to Dalla Vecchia & Schaye (2012) -- MW analogue (Mgas ~ 109 Mʘ Ngas = 105) & Dwarf

Keller+ 2014

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SLIDE 16

MW Analogue: Temperature & Column Density

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SLIDE 17

MW & Dwarf Star Formation

Keller+ 2014

  • Star formation rates
  • regulated. Bursty as

expected in dwarf

  • Higher mass loading
  • Outflow evolution

similar to Dalla Vecchia & Schaye 2012

  • Note: dwarf has low

surface density

  • Kennicutt-Schmidt law

matched

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SLIDE 18

Galaxies: SFR & Outflows

Milky Way Dwarf

Keller+ 2014

Outflow Rate & SFR Outflow Velocity Time (Myr) Time (Myr)

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SLIDE 19

Temperature-Density Phase space

No gas in short cooling time region Particles split into cold dense + hot rarefied phases Rapidly become hot, single phase – evolve adiabatically

Keller+ 2014

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SLIDE 20

Summary

  • Superbubble is relevant scale for stellar feedback in galaxies
  • Thermal conduction is dominant physical process in

superbubble evolution

  • Taking this into account gives you a powerful model for

feedback:

– Separating Cold & Hot phases in unresolved superbubble prevents

  • vercooling

– Feedback can be continuous, multi-source – Feedback gas doesn’t persist in unphysical phases – Star formation is strongly regulated, winds are driven with realistic mass loadings

  • Read the Paper:

– astro-ph/1405.2625 (Accepted MNRAS) – Keller, Wadsley, Benincasa & Couchman 2014

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SLIDE 21

Stellar Feedback Budget

Starburst ‘99 Erg per Mʘ

Time (years) Bolometric Luminosity Supernovae Type II Winds UV Energy Injection Rate (log10 erg/s/Mʘ)

  • UV & Radiation

pressure disrupt dense clouds

– Denser gas (>104 H/cc) dispersed, star formation cut off

  • SNII and stellar winds

Steady 1034 erg/s/Mʘ

for ~ 40 Myr

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SLIDE 22

Super bubbles: Vishniac Instabilities

Theory: Vishniac 1983 Sims: McLeod & Whitworth 2013, Nayakshin+ 2012 (AGN) Nirvana simulations 3 star bubble Krause et al 2013

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SLIDE 23

Super bubbles: X-Ray Observations

Chu 2008

Krause+ 2014

  • X-Ray luminosity highly

variable over space, time

  • Very few observations,

large scatter in observed LX

  • Leaking of interior, B-

field amplification in shell may explain some reduced luminosities (see Rosen+ 2014)

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SLIDE 24

Clumpy medium

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SLIDE 25

Clumpy Medium

  • Some changes in bubble mass/momentum
  • Agreement with direct model still good
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SLIDE 26

Reduced Conduction & Magnetic Fields

  • Conduction

suppressed across magnetic field lines

  • 100x reduction in

conduction rate κ0 results in only factor of ~2 reduction in Mb

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SLIDE 27

Multiphase Properties

  • Median time as mixed-phase particle < 5 Myr
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SLIDE 28

Cosmological Galaxy (now z=2)

  • ~ 10 11 Msun halo
  • So far on track for reasonable M *

Coming Soon…